Apparatus and method for measuring optical characteristics of an object

ABSTRACT

Color measuring systems and methods are disclosed. Perimeter receiver fiber optics are spaced apart from a central source fiber optic and receive light reflected from the surface of the object being measured. Light from the perimeter fiber optics pass to a variety of filters. The system utilizes the perimeter receiver fiber optics to determine information regarding the height and angle of the probe with respect to the object being measured. Under processor control, the color measurement may be made at a predetermined height and angle. Various color spectral photometer arrangements are disclosed. Translucency, fluorescence and/or surface texture data also may be obtained. Audio feedback may be provided to guide operator use of the system. The probe may have a removable or shielded tip for contamination prevention.

This application is a continuation of application Ser. No. 08/909,989filed on Aug. 12, 1997, now U.S. Pat. No. 5,883,708.

FIELD OF THE INVENTION

The present invention relates to devices and methods for measuring thecolor of objects, and more particularly to devices and methods formeasuring the color of teeth, fabric or other objects or surfaces with ahand-held probe that presents minimal problems with height or angulardependencies.

BACKGROUND OF THE INVENTION

Various color measuring devices such as spectrophotometers andcalorimeters are known in the art. To understand the limitations of suchconventional devices, it is helpful to understand certain principlesrelating to color. Without being bound by theory, Applicants provide thefollowing discussion.

The color of an object determines the manner in which light is reflectedfrom the surface of the object. When light is incident upon an object,the reflected light will vary in intensity and wavelength dependent uponthe color of the surface of the object. Thus, a red object will reflectred light with a greater intensity than a blue or a green object, andcorrespondingly a green object will reflect green light with a greaterintensity than a red or blue object.

One method of quantifying the color of an object is to illuminate itwith broad band spectrum or “white” light, and measure the spectralproperties of the reflected light over the entire visible spectrum andcompare the reflected spectrum with the incident light spectrum. Suchinstruments typically require a broad band spectrophotometer, whichgenerally are expensive, bulky and relatively cumbersome to operate,thereby limiting the practical application of such instruments.

For certain applications, the broad band data provided by aspectrophotometer is unnecessary. For such applications, devices havebeen produced or proposed that quantify color in terms of a numericalvalue or relatively small set of values representative of the color ofthe object.

It is known that the color of an object can be represented by threevalues. For example, the color of an object can be represented by red,green and blue values, an intensity value and color difference values,by a CIE value, or by what are known as “tristimulus values” or numerousother orthogonal combinations. It is important that the three values beorthogonal; i.e., any combination of two elements in the set cannot beincluded in the third element.

One such method of quantifying the color of an object is to illuminatean object with broad band “white” light and measure the intensity of thereflected light after it has been passed through narrow band filters.Typically three filters (such as red, green and blue) are used toprovide tristimulus light values representative of the color of thesurface. Yet another method is to illuminate an object with threemonochromatic light sources (such as red, green and blue) one at a timeand then measure the intensity of the reflected light with a singlelight sensor. The three measurements are then converted to a tristimulusvalue representative of the color of the surface. Such color measurementtechniques can be utilized to produce equivalent tristimulus valuesrepresentative of the color of the surface. Generally, it does notmatter if a “white” light source is used with a plurality of colorsensors (or a continuum in the case of a spectrophotometer), or if aplurality of colored light sources are utilized with a single lightsensor.

There are, however, difficulties with the conventional techniques. Whenlight is incident upon a surface and reflected to a light receiver, theheight of the light sensor and the angle of the sensor relative to thesurface and to the light source also affect the intensity of thereceived light. Since the color determination is being made by measuringand quantifying the intensity of the received light for differentcolors, it is important that the height and angular dependency of thelight receiver be eliminated or accounted for in some manner.

One method for eliminating the height and angular dependency of thelight source and receiver is to provide a fixed mounting arrangementwhere the light source and receiver are stationary and the object isalways positioned and measured at a preset height and angle. The fixedmounting arrangement greatly limits the applicability of such a method.Another method is to add mounting feet to the light source and receiverprobe and to touch the object with the probe to maintain a constantheight and angle. The feet in such an apparatus must be wide enoughapart to insure that a constant angle (usually perpendicular) ismaintained relative to the object. Such an apparatus tends to be verydifficult to utilize on small objects or on objects that are hard toreach, and in general does not work satisfactorily in measuring objectswith curved surfaces.

The use of color measuring devices in the field of dentistry has beenproposed. In modern dentistry, the color of teeth typically arequantified by manually comparing a patient's teeth with a set of “shadeguides.” There are numerous shade guides available for dentists in orderto properly select the desired color of dental prosthesis. Such shadeguides have been utilized for decades and the color determination ismade subjectively by the dentist by holding a set of shade guides nextto a patient's teeth and attempting to find the best match.Unfortunately, however, the best match often is affected by the ambientlight color in the dental operatory and the surrounding color of thepatient's makeup or clothing and by the fatigue level of the dentist.

Similar subjective color quantification also is made in the paintindustry by comparing the color of an object with a paint referenceguide. There are numerous paint guides available in the industry and thecolor determination also often is affected by ambient light color, userfatigue and the color sensitivity of the user. Many individuals arecolor insensitive (color blind) to certain colors, further complicatingcolor determination.

In general, color quantification is needed in many industries. Several,but certainly not all, applications include: dentistry (color of teeth);dermatology (color of skin lesions); interior decorating (color ofpaint, fabrics); the textile industry; automotive repair (matching paintcolors); photography (color of reproductions, color reference ofphotographs to the object being photographed); printing and lithography;cosmetics (hair and skin color, makeup matching); and other applicationsin which it useful to measure color in an expedient and reliable manner.

With respect to such applications, however, the limitations ofconventional color measuring techniques typically restrict the utilityof such techniques. For example, the high cost and bulkiness of typicalbroad band spectrometers, and the fixed mounting arrangements or feetrequired to address the height and angular dependency, often limit theapplicability of such conventional techniques

Moreover, another limitation of such conventional methods and devicesare that the resolution of the height and angular dependency problemstypically require contact with the object being measured. In certainapplications, it may be desirable to measure and quantify the color ofan object with a small probe that does not require contact with thesurface of the object. In certain applications, for example, hygienicconsiderations make such contact undesirable. In the other applicationssuch as interior decorating, contact with the object can mar the surface(such as if the object is coated with wet paint) or otherwise causeundesirable effects.

In summary, there is a need for a low cost, hand-held probe of smallsize that can reliably measure and quantify the color of an objectwithout requiring physical contact with the object, and also a need formethods based on such a device in the field of dentistry and otherapplications.

SUMMARY OF THE INVENTION

In accordance with the present invention, devices and methods areprovided for measuring the color of objects, reliably and with minimalproblems of height and angular dependence. A handheld probe is utilizedin the present invention, with the handheld probe containing a number offiber optics. Light is directed from one (or more) light source fiberoptics towards the object to be measured, which in certain preferredembodiments is a central light source fiber optic (other light sourcearrangements also may be utilized). Light reflected from the object isdetected by a number of light receiver fiber optics. Included in thelight receiver fiber optics are a plurality of perimeter fiber optics.In certain preferred embodiments, three perimeter fiber optics areutilized in order to take measurements at a desired, and predeterminedheight and angle, thereby minimizing height and angular dependencyproblems found in conventional methods. In certain embodiments, thepresent invention also may measure translucence and fluorescencecharacteristics of the object being measured, as well as surface textureand/or other surface characteristics.

The present invention may include constituent elements of a broad bandspectrophotometer, or, alternatively, may include constituent elementsof a tristimulus type calorimeter. The present invention may employ avariety of color measuring devices in order to measure color in apractical, reliable and efficient manner, and in certain preferredembodiments includes a color filter array and a plurality of colorsensors. A microprocessor is included for control and calculationpurposes. A temperature sensor is included to measure temperature inorder to detect abnormal conditions and/or to compensate for temperatureeffects of the filters or other components of the system. In addition,the present invention may include audio feedback to guide the operatorin making color measurements, as well as one or more display devices fordisplaying control, status or other information.

With the present invention, color measurements may be made with ahandheld probe in a practical and reliable manner, essentially free ofheight and angular dependency problems, without resorting to fixtures,feet or other undesirable mechanical arrangements for fixing the heightand angle of the probe with respect to the object.

Accordingly, it is an object of the present invention to addresslimitations of conventional color measuring techniques.

It is another object of the present invention to provide a method anddevice useful in measuring the color of teeth, fabric or other objectsor surfaces with a hand-held probe of practical size that does notrequire contact with the object or surface.

It is a further object of the present invention to provide a colormeasurement probe and method that does not require fixed positionmechanical mounting, feet or other mechanical impediments.

It is yet another object of the present invention to provide a probe andmethod useful for measuring color that may be utilized with a probesimply placed near the surface to be measured.

It is a still further object of the present invention to provide a probeand method that are capable of determining translucency characteristicsof the object being measured.

It is a further object of the present invention to provide a probe andmethod that are capable of determining surface texture characteristicsof the object being measured.

It is a still further object of the present invention to provide a probeand method that are capable of determining fluorescence characteristicsof the object being measured.

Finally, it is an object of the present invention to provide a probe andmethod that can measure the area of a small spot singulary, or that alsocan measure irregular shapes by moving the probe over an area andintegrating the color of the entire area.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention may be more fully understood by a description ofcertain preferred embodiments in conjunction with the attached drawingsin which:

FIG. 1 is a diagram illustrating a preferred embodiment of the presentinvention;

FIG. 2 is a diagram illustrating a cross section of a probe inaccordance with a preferred embodiment of the present invention;

FIG. 3 is a diagram illustrating an arrangement of fiber optic receiversand sensors utilized with a preferred embodiment of the presentinvention;

FIGS. 4A to 4C illustrate certain geometric considerations of fiberoptics;

FIGS. 5A and 5B illustrate the light amplitude received by fiber opticlight receivers as a function of height from an object;

FIG. 6 is a flow chart illustrating a color measuring method inaccordance with an embodiment of the present invention;

FIGS. 7A and 7B illustrate a protective cap that may be used withcertain embodiments of the present invention;

FIGS. 8A and 8B illustrate removable probe tips that may be used withcertain embodiments of the present invention;

FIG. 9 illustrates a fiber optic bundle in accordance with anotherpreferred embodiment of the present invention;

FIGS. 10A, 10B, 10C and 10D illustrate and describe other fiber opticbundle configurations that may be used in accordance with yet otherpreferred embodiments of the present invention;

FIG. 11 illustrates a linear optical sensor array that may be used incertain embodiments of the present invention;

FIG. 12 illustrates a matrix optical sensor array that may be used incertain embodiments of the present invention;

FIGS. 13A and 13B illustrate certain optical properties of a filterarray that may be used in certain embodiments of the present invention;

FIGS. 14A and 14B illustrate examples of received light intensities ofreceivers used in certain embodiments of the present invention; and

FIG. 15 is a flow chart illustrating audio tones that may be used incertain preferred embodiments of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

The present invention will be described in greater detail with referenceto certain preferred embodiments.

With reference to FIG. 1, an exemplary preferred embodiment of a colormeasuring system and method in accordance with the present inventionwill be described.

Probe tip 1 encloses a plurality of fiber optics, each of which mayconstitute one or more fiber optic fibers. In a preferred embodiment,the fiber optics contained within probe tip 1 includes a single lightsource fiber optic and three light receiver fiber optics. The use ofsuch fiber optics to measure the color of an object will be describedlater herein. Probe tip 1 is attached to probe body 2, on which is fixedswitch 17. Switch 17 communicates with microprocessor I0 through wire 18and provides, for example, a mechanism by which an operator may activatethe device in order to make a color measurement. Fiber optics withinprobe tip 1 terminate at the forward end thereof (i.e., the end awayfrom probe body 2). The forward end of probe tip 1 is directed towardsthe surface of the object to be measured as described more fully below.The fiber optics within probe tip 1 optically extend through probe body2 and through fiber optic cable 3 to light sensors 8, which are coupledto microprocessor 10.

It should be noted that microprocessor 10 includes conventionalassociated components, such as memory (programmable memory, such asPROM, EPROM or EEPROM; working memory such as DRAMs or SRAMs; and/orother types of memory such as non-volatile memory, such as FLASH),peripheral circuits, clocks and power supplies, although for claritysuch components are not explicitly shown. Other types of computingdevices (such as other microprocessor systems, programmable logic arraysor the like) are used in other embodiments of the present invention.

In the embodiment of FIG. 1, the fiber optics from fiber optic cable 3end at splicing connector 4. From splicing connector 4, each of thethree receiver fiber optics used in this embodiment is spliced into atleast five smaller fiber optics (generally denoted as fibers 7), whichin this embodiment are fibers of equal diameter, but which in otherembodiments may be of unequal diameter (such as a larger or smaller“height/angle” or perimeter fiber, as more fully described herein). Oneof the fibers of each group of five fibers passes to light sensors 8through a neutral density filter (as more fully described with referenceto FIG. 3), and collectively such neutrally filtered fibers are utilizedfor purposes of height/angle determination (and also may be utilized tomeasure surface characteristics, as more fully described herein). Fourof the remaining fibers of each group of fibers passes to light sensors8 through color filters and are used to make the color measurement. Instill other embodiments, splicing connector 4 is not used, and fiberbundles of, for example, five or more fibers each extend from lightsensors 8 to the forward end of probe tip 1. In certain embodiments,unused fibers or other materials may be included as part of a bundle offibers for purposes of, for example, easing the manufacturing processfor the fiber bundle. What should be noted is that, for purposes of thepresent invention, a plurality of light receiver fiber optics (such asfibers 7) are presented to light sensors 8, with the light from thelight receiver fiber optics representing light reflected from object 20.While the various embodiments described herein present tradeoffs andbenefits that may not have been apparent prior to the present invention(and thus may be independently novel), what is important for the presentdiscussion is that light from fiber optics at the forward end of probetip 1 is presented to color sensors 8 for color measurement andangle/height determination, etc.

Light source 11 in the preferred embodiment is a halogen light source(of, for example, 5-100 watts, with the particular wattage chosen forthe particular application), which may be under the control ofmicroprocessor 10. The light from light source 11 reflects from coldmirror 6 and into source fiber optic 5. Source fiber optic 5 passesthrough to the forward end of probe tip 1 and provides the lightstimulus used for purposes of making the measurements described herein.Cold mirror 6 reflects visible light and passes infra-red light, and isused to reduce the amount of infra-red light produced by light source 11before the light is introduced into source fiber optic 5. Such infra-redlight reduction of the light from a halogen source such as light source11 can help prevent saturation of the receiving light sensors, which canreduce overall system sensitivity. Fiber 15 receives light directly fromlight source 11 and passes through to light sensors 8 (which may bethrough a neutral density filter). Microprocessor 10 monitors the lightoutput of light source 11 through fiber 15, and thus may monitor and, ifnecessary compensate for, drift of the output of light source 11. Incertain embodiments, microprocessor 10 also may sound an alarm (such asthrough speaker 16) or otherwise provide some indication if abnormal orother undesired performance of light source 11 is detected.

The data output from light sensors 8 pass to microprocessor 10.Microprocessor 10 processes the data from light sensors 8 to produce ameasurement of color and/or other characteristics. Microprocessor 10also is coupled to key pad switches 12, which serve as an input device.Through key pad switches 12, the operator may input control informationor commands, or information relating to the object being measured or thelike. In general, key pad switches 12, or other suitable data inputdevices (such as push button, toggle, membrane or other switches or thelike), serve as a mechanism to input desired information tomicroprocessor 10.

Microprocessor 10 also communicates with UART 13, which enablesmicroprocessor 10 to be coupled to an external device such as computer13A. In such embodiments, color data provided by microprocessor 10 maybe processed as desired for the particular application, such as foraveraging, format conversion or for various display or print options,etc. In the preferred embodiment, UART 13 is configured so as to providewhat is known as a RS232 interface, such as is commonly found inpersonal computers.

Microprocessor 10 also communicates with LCD 14 for purposes ofdisplaying status, control or other information as desired for theparticular application. For example, color bars, charts or other graphicrepresentations of the color or other collected data and/or the measuredobject or tooth may be displayed In other embodiments, other displaydevices are used, such as CRTs, matrix-type LEDs, lights or othermechanisms for producing a visible indicia of system status or the like.Upon system initialization, for example, LCD 14 may provide anindication that the system is stable, ready and available for takingcolor measurements.

Also coupled to microprocessor 10 is speaker 16. Speaker 16, in apreferred embodiment as discussed more fully below, serves to provideaudio feedback to the operator, which may serve to guide the operator inthe use of the device. Speaker 16 also may serve to provide status orother information alerting the operator of the condition of the system,including an audio tone, beeps or other audible indication (i.e., voice)that the system is initialized and available for taking measurements.Speaker 16 also may present audio information indicative of the measureddata, shade guide or reference values corresponding to the measureddata, or an indication of the status of the color measurements.

Microprocessor 10 also receives an input from temperature sensor 9.Given that many types of filters (and perhaps light sources or othercomponents) may operate reliably only in a given temperature range,temperature sensor 9 serves to provide temperature information tomicroprocessor 10. In particular, color filters, such as may be includedin light sensors 8, are sensitive to temperature, and operate reliablyonly over a certain temperature range. In certain embodiments, if thetemperature is within a usable range, microprocessor 10 may compensatefor temperature variations of the color filters. In such embodiments,the color filters are characterized as to filtering characteristics as afunction of temperature, either by data provided by the filtermanufacturer, or through measurement as a function of temperature. Suchfilter temperature compensation data may be stored in the form of alook-up table in memory, or may be stored as a set of polynomialcoefficients from which the temperature characteristics of the filtersmay be computed by microprocessor 10.

In general, under control of microprocessor 10, which may be in responseto operator activation (through, for example, key pad switches 12 orswitch 17), light is directed from light source 11, and reflected fromcold mirror 6 through source fiber optic 5 (and through fiber opticcable 3, probe body 2 and probe tip 1) and is directed onto object 20.Light reflected from object 20 passes through the receiver fiber opticsin probe tip 1 to light sensors 8 (through probe body 2, fiber opticcable 3 and fibers 7). Based on the information produced by lightsensors B, microprocessor 10 produces a color measurement result orother information to the operator. Color measurement or other dataproduced by microprocessor 10 may be displayed on display 14, passedthrough UART 13 to computer 13A, or used to generate audio informationthat is presented to speaker 16: Other operational aspects of thepreferred embodiment illustrated in FIG. 1 will be explainedhereinafter.

With reference to FIG. 2, a preferred embodiment of the fiber opticarrangement presented at the forward end of probe tip 1 will now bedescribed. As illustrated in FIG. 2, a preferred embodiment of thepresent invention utilizes a single central light source fiber optic,denoted as light source fiber optic S, and a plurality of perimeterlight receiver fiber optics, denoted as light receivers R1, R2 and R3.As is illustrated, a preferred embodiment of the present inventionutilizes three perimeter fiber optics, although in other embodimentstwo, four or some other number of receiver fiber optics are utilized. Asmore fully described herein, the perimeter light receiver fiber opticsserve not only to provide reflected light for purposes of making thecolor measurement, but such perimeter fibers also serve to provideinformation regarding the angle and height of probe tip 1 with respectto the surface of the object that is being measured, and also mayprovide information regarding the surface characteristics of the objectthat is being measured.

In the illustrated preferred embodiment, receiver fiber optics R1 to R3are positioned symmetrically around source fiber optic S, with a spacingof about 120 degrees from each other. It should be noted that spacing tis provided between receiver fiber optics R1 to R3 and source fiberoptic S. While the precise angular placement of the receiver fiberoptics around the perimeter of the fiber bundle in general is notcritical, it has been determined that three receiver fiber opticspositioned 120 degrees apart generally may give acceptable results. Asdiscussed above, in certain embodiments light receiver fiber optics R1to R3 each constitute a single fiber, which is divided at splicingconnector 4 (refer again to FIG. 1), or, in alternate embodiments, lightreceiver fiber optics R1 to R3 each constitute a bundle of fibers,numbering, for example, at least five fibers per bundle. It has beendetermined that, with available fibers of uniform size, a bundle of, forexample, seven fibers may be readily produced (although as will beapparent to one of skill in the art, the precise number of fibers may bedetermined in view of the desired number of receiver fiber optics,manufacturing considerations, etc.). The use of light receiver fiberoptics R1 to R3 to produce color measurements in accordance with thepresent invention is further described elsewhere herein, although it maybe noted here that receiver fiber optics R1 to R3 may serve to detectwhether, for example, the angle of probe tip 1 with respect to thesurface of the object being measured is at 90 degrees, or if the surfaceof the object being measured contains surface texture and/or spectralirregularities. In the case where probe tip 1 is perpendicular to thesurface of the object being measured and the surface of the object beingmeasured is a diffuse reflector, then the light intensity input into theperimeter, fibers should be approximately equal. It also should be notedthat spacing t serves to adjust the optimal height at which colormeasurements should be made (as more fully described below), and alsoensures that the light reflected into receiver fiber optics R1 to R3 isat an angle for diffuse reflection, which helps to reduce problemsassociated with measurements of “hot spots” on the surface of the objectbeing measured.

In one particular aspect of the present invention, area between thefiber optics on probe tip 1 may be wholly or partially filled with anon-reflective material and/or surface (which may be a black mat,contoured or other non-reflective surface). Having such exposed area ofprobe tip 1 non-reflective helps to reduce undesired reflections,thereby helping to increase the accuracy and reliability of the presentinvention.

With reference to FIG. 3, a partial arrangement of light receiver fiberoptics and sensors used in a preferred embodiment of the presentinvention will now be described. Fibers 7 represent light receivingfiber optics, which transmit light reflected from the object beingmeasured to light sensors 8. In a preferred embodiment, sixteen sensors(two sets of eight) are utilized, although for ease of discussion only 8are illustrated in FIG. 3 (in this preferred embodiment, the circuitryof FIG. 3 is duplicated, for example, in order to result in sixteensensors). In other embodiments, other numbers of sensors are utilized inaccordance with the present invention.

Light from fibers 7 is presented to sensors 8, which in a preferredembodiment pass through filters 22 to sensing elements 24. In thispreferred embodiment, sensing elements 24 include light-to-frequencyconverters, manufactured by Texas Instruments and sold under the partnumber TSL230. Such converters constitute, in general, photo diodearrays that integrate the light received from fibers 7 and output an ACsignal with a frequency proportional to the intensity (not frequency) ofthe incident light. Without being bound by theory, the basic principleof such devices is that, as the intensity increases, the integratoroutput voltage rises more quickly, and the shorter the integrator risetime, the greater the output frequency. The outputs of the TSL230sensors are TTL or CMOS compatible digital signals, which may be coupledto various digital logic devices.

The outputs of sensing elements 24 are, in this embodiment, asynchronoussignals of frequencies depending upon the light intensity presented tothe particular sensing elements, which are presented to processor 26. Ina preferred embodiment, processor 26 is a Microchip PIC16C55microprocessor, which as described more fully herein implements analgorithm to measure the frequencies of the signals output by sensingelements 24.

As previously described, processor 26 measures the frequencies of thesignals output from sensing elements 24. In a preferred embodiment,processor 26 implements a software timing loop, and at periodicintervals processor 26 reads the states of the outputs of sensingelements 24. An internal counter is incremented each pass through thesoftware timing loop. The accuracy of the timing loop generally isdetermined by the crystal oscillator time base (not shown in FIG. 3)coupled to processor 26 (such oscillators typically are quite stable).After reading the outputs of sensing elements 24, processor 26 performsan exclusive OR (“XOR”) AU operation with the last data read (in apreferred embodiment such data is read in byte length). If any bit haschanged, the XOR operation will produce a 1, and, if no bits havechanged, the XOR operation will produce a 0. If the result is non-zero,the input byte is saved along with the value of the internal counter(that is incremented each pass through the software timing loop). If theresult is zero, the systems waits (e.g., executes no operationinstructions) the same amount of time as if the data had to be saved,and the looping operation continues. The process continues until alleight inputs have changed at least twice, which enables measurement of afull ½ period of each input. Upon conclusion of the looping process,processor 26 analyzes the stored input bytes and internal counterstates. There should be 2 to 16 saved inputs (for the 8 total sensors ofFIG. 3) and counter states (if two or more inputs change at the sametime, they are saved simultaneously). As will be understood by one ofskill in the art, the stored values of the internal counter containsinformation determinative of the period of the signals received fromsensing elements 24. By proper subtraction of internal counter values attimes when an input bit has changed, the period may be calculated. Suchperiods calculated for each of the outputs of sensing elements isprovided by processor 26 to microprocessor 10 (see, e.g., FIG. 1). Fromsuch calculated periods, a measure of the received light intensities maybe calculated.

It should be noted that the sensing circuitry and methodologyillustrated in FIG. 3 have been determined to provide a practical andexpedient manner in which to measure the light intensities received bysensing elements 24. In other embodiments, other circuits andmethodologies are employed (other exemplary sensing schemes aredescribed elsewhere herein).

As discussed above with reference to FIG. 1, one of fibers 7 measureslight source 11, which may be through a neutral density filter, whichserves to reduce the intensity of the received light in order maintainthe intensity roughly in the range of the other received lightintensities. Three of fibers 7 also are from perimeter receiver fiberoptics R1 to R3 (see, e.g., FIG. 2) and also may pass through neutraldensity filters. Such receiving fibers 7 serve to provide data fromwhich angle/height information and/or surface characteristics may bedetermined.

The remaining twelve fibers (of the preferred embodiment's total of 16fibers) of fibers 7 pass through color filters and are used to producethe color measurement. In a preferred embodiment, the color filters areKodak Sharp Cutting Wratten Gelatin Filters, which pass light withwavelengths greater than the cutoff value of the filter (i.e., redishvalues), and absorb light with wavelengths less than the cut-off valueof the filter (i.e., bluish values). “Sharp Cutting” filters areavailable in a wide variety of cut-off frequencies/wavelengths, and thecut-off values generally may be selected by proper selection of thedesired cutoff filter. In a preferred embodiment, the filter cut-offvalues are chosen to cover the entire visible spectrum and, in general,to have band spacings of approximately the visible band range (or otherdesired range) divided by the number of receivers/filters. As anexample, 700 nanometers minus 400 nanometers, divided by 11 bands(produced by twelve color receivers/sensors), is roughly 30 nanometerband spacing.

With an array of cut-off filters as described above, and without beingbound by theory or the specific embodiments described herein, thereceived optical spectrum may be measured/calculated by subtracting thelight intensities of “adjacent” color receivers. For example, band 1(400 nm to 430 nm)=(intensity of receiver 12) minus (intensity ofreceiver 11), and so on for the remaining bands. Such an array of cutofffilters, and the intensity values that may result from filtering withsuch an array, are more fully described in connection with FIGS. 13A to14B.

In a preferred embodiment of the present invention, the specificcharacteristics of the light source, filters, sensors and fiber optics,etc., are normalized/calibrated by directing the probe towards, andmeasuring, a known color standard. Such normalization/calibration may beperformed by placing the probe in a suitable fixture, with the probedirected from a predetermined position (i.e., height and angle) from theknown color standard. Such measured normalization/calibration data maybe stored, for example, in a look-up table, and used by microprocessor10 to normalize or correct measured color or other data. Such proceduresmay be conducted at start-up, at regular periodic intervals, or byoperator command, etc.

What should be noted from the above description is that the receivingand sensing fiber optics and circuitry illustrated in FIG. 3 provide apractical and expedient way to determine the intensity by color of thelight reflected from the surface of the object being measured.

It also should be noted that such a system measures the spectral band ofthe reflected light from the object, and once measured such spectraldata may be utilized in a variety of ways. For example, such spectraldata may be displayed directly as intensity-wavelength band values. Inaddition, tristimulus type values may be readily computed (through, forexample, conventional matrix math), as may any other desired colorvalues. In one particular embodiment useful in dental applications (suchas for dental prostheses), the color data is output in the form of aclosest match or matches of dental shade guide value(s). In a preferredembodiment, various existing shade guides (such as the shade guidesproduced by Vita Zahnfabrik) are characterized and stored in a look-uptable, and the color measurement data arc used to select the closestshade guide value. In still other embodiments, the color measurementdata are used (such as with look-up tables) to select materials for thecomposition of paint or ceramics such as for prosthetic teeth. There aremany other uses of such spectral data measured in accordance with thepresent invention.

It is known that certain objects such as human teeth may fluoresce, andsuch characteristics also may be measured in accordance with the presentinvention. A light source with an ultraviolet component may be used toproduce more accurate color data of such objects. In certainembodiments, a tungsten/halogen source (such as used in a preferredembodiment) may be combined with a UV light source (such as a mercuryvapor, xenon or other fluorescent light source, etc.) to produce a lightoutput capable of causing the object to fluoresce Alternately, aseparate UV light source, combined with a visible-light-blocking filter,may be used to illuminate the object. Such a UV light source may becombined with light from a red LED (for example) in order to provide avisual indication of when the UV light is on and also to serve as an aidfor the directional positioning of the probe operating with such a lightsource. A second measurement may be taken using the UV light source in amanner analogous to that described earlier, with the band of the red LEDor other supplemental light source being ignored. The second measurementmay thus be used to produce an indication of the fluorescence of thetooth or other object being measured. With such a UV light source, asilica fiber optic (or other suitable material) typically would berequired to transmit the light to the object (standard fiber opticmaterials such as glass and plastic do not propagate UV light in adesired manner, etc.).

As described earlier, the present invention utilizes a plurality ofperimeter receiver fiber optics spaced apart from and around a centralsource fiber optic to measure color and determine information regardingthe height and angle of the probe with respect to the surface of theobject being measured, which may include surface characteristicinformation, etc. Without being bound by theory, a principle underlyingthis aspect of the present invention will now be described withreference to FIGS. 4A to 4C.

FIG. 4A illustrates a typical step index fiber optic consisting of acore and a cladding. For this discussion, it is assumed that the corehas an index of refraction of no and the cladding has an index ofrefraction of n₁. Although the following discussion is directed to “stepindex” fibers, it will be appreciated by those of skill in the art thatsuch discussion generally is applicable for gradient index fibers aswell.

In order to propagate light without loss, the light must be incidentwithin the core of the fiber optic at an angle greater than the criticalangle, which may be represented as Sin⁻¹ {n₁/n₀}, where n₀ is the indexof refraction of the core and n₁ is the index of refraction of thecladding. Thus, all light must enter the fiber at an acceptance angleequal to or less than phi, with phi=2×Sin⁻¹ {(n₀ ²−n₁ ²)}, or it willnot be propagated in a desired manner.

For light entering a fiber optic, it must enter within the acceptanceangle phi. Similarly, when the light exits a fiber optic, it will exitthe fiber optic within a cone of angle phi as illustrated in FIG. 4A.The value (n₀ ²−n₁ ²) is referred to as the aperture of the fiber optic.For example, a typical fiber optic may have an aperture of 0.5, and anacceptance angle of 60°.

Consider using a fiber optic as a light source. One end is illuminatedby a light source (such as light source 11 of FIG. 1), and the other isheld near a surface. The fiber optic will emit a cone of light asillustrated in FIG. 4A. If the fiber optic is held perpendicular to asurface it will create a circular light pattern on the surface. As thefiber optic is raised, the radius r of the circle will increase. As thefiber optic is lowered, the radius of the light pattern will decrease.Thus, the intensity of the light (light energy per unit area) in theilluminated circular area will increase as the fiber optic is loweredand will decrease as the fiber optic is raised.

The same principle generally is true for a fiber optic being utilized asa receiver. Consider mounting a light sensor on one end of a fiber opticand holding the other end near an illuminated surface. The fiber opticcan only propagate light without loss when the light entering the fiberoptic is incident on the end of the fiber optic near the surface if thelight enters the fiber optic within its acceptance angle phi. A fiberoptic utilized as a light receiver near a surface will only accept andpropagate light from the circular area of radius r on the surface. Asthe fiber optic is raised from the surface, the area increases. As thefiber optic is lowered to the surface, the area decreases.

Consider two fiber optics parallel to each other as illustrated in FIG.4B. For simplicity of discussion, the two fiber optics illustrated areidentical in size and aperture. The following discussion, however,generally would be applicable for fiber optics that differ in size andaperture. One fiber optic is a source fiber optic, the other fiber opticis a receiver fiber optic. As the two fiber optics are heldperpendicular to a surface, the source fiber optic emits a cone of lightthat illuminates a circular area of radius r. The receiver fiber opticcan only accept light that is within its acceptance angle phi, or onlylight that is received within a cone of angle phi. If the only lightavailable is that emitted by the source fiber optic, then the only lightthat can be accepted by the receiver fiber optic is the light thatstrikes the surface at the intersection of the two circles asillustrated in FIG. 4C. As the two fiber optics are lifted from thesurface, the proportion of the intersection of the two circular areasrelative to the circular area of the source fiber optic increases. Asthey near the surface, the proportion of the intersection of the twocircular areas to the circular area of the source fiber optic decreases.If the fiber optics are held too close to the surface, the circularareas will no longer intersect and no light emitted from the sourcefiber optic will be received by the receiver fiber optic.

As discussed earlier, the intensity of the light in the circular areailluminated by the source fiber increases as the fiber is lowered to thesurface. The intersection of the two cones, however, decreases as thefiber optic pair is lowered. Thus, as the fiber optic pair is lowered toa surface, the total intensity of light received by the receiver fiberoptic increases to a maximal value, and then decreases sharply as thefiber optic pair is lowered still further to the surface. Eventually,the intensity will decrease essentially to zero (assuming the objectbeing measured is not translucent, as described more fully herein), andwill remain essentially zero until the fiber a optic pair is in contactwith the surface. Thus, as a source-receiver pair of fiber optics asdescribed above are positioned near a surface and as their height isvaried, the intensity of light received by the receiver fiber opticreaches a maximal value at a critical height h_(c).

Again without being bound by theory, an interesting property of thecritical height h_(c) has been observed. The critical height h_(c) is afunction primarily of the geometry of fixed parameters, such as fiberapertures, fiber diameters and fiber spacing. Since the receiver fiberoptic in the illustrated arrangement is only detecting a maximum valueand not attempting to quantify the value, its maximum is independent ofthe surface characteristics It is only necessary that the surfacereflect sufficient light from the intersecting area of the source andreceiver fiber optics to be within the detection range of the receiverfiber optic light sensor. Thus, red or green or blue or any colorsurface will all exhibit a maximum at the same critical height h_(c).Similarly, smooth reflecting surfaces and rough surfaces also will havevarying intensity values at the maximal value, but generally speakingall such surfaces will exhibit a maximum at the same critical heighth_(c). The actual value of the light intensity will be a function of thecolor of the surface and of the surface characteristics, but the heightwhere the maximum intensity value occurs in general will not.

Although the above discussion has focused on two fiber opticsperpendicular to a surface, similar analysis is applicable for fiberoptic pairs at other angles. When a fiber optic is not perpendicular toa surface, it generally illuminates an elliptical area. Similarly, theacceptance area of a receiver fiber optic generally becomes elliptical.As the fiber optic pair is moved closer to the surface, the receiverfiber optic also will detect a maximal value at a critical heightindependent of the surface color or characteristics. The maximalintensity value measured when the fiber optic pair is not perpendicularto the surface, however, will be less than the maximal intensity valuemeasured when the fiber optic pair is perpendicular to the surface.

Referring now to FIGS. 5A and 5B, the intensity of light received as afiber optic source-receiver pair is moved to and from a surface will nowbe described. FIG. 5A illustrates the intensity of the received light asa function of time. Corresponding FIG. 5B illustrates the height of thefiber optic pair from the surface of the object being measured. FIGS. 5Aand 5B illustrate (for ease of discussion) a relatively uniform rate ofmotion of the fiber optic pair to and from the surface of the objectbeing measured (although similar illustrations/analysis would beapplicable for non-uniform rates as well).

FIG. 5A illustrates the intensity of received light as the fiber opticpair is moved to and then from a surface. While FIG. 5A illustrates theintensity relationship for a single receiver fiber optic, similarintensity relationships would be expected to be observed for otherreceiver fiber optics, such as, for example, the multiple receiver fiberoptics of FIGS. 1 and 2. In general with the preferred embodimentdescribed above, all fifteen fiber optic receivers (of fibers 7) willexhibit curves similar to that illustrated in FIG. 5A.

FIG. 5A illustrates five regions. In region 1, the probe is movedtowards the surface of the object being measured, which causes thereceived light intensity to increase. In region 2, the probe is movedpast the critical height, and the received light intensity peaks andthen falls off sharply. In region 3, the probe essentially is in contactwith the surface of the object being measured. As illustrated, thereceived intensity in region 3 will vary depending upon the translucenceof the object being measured. If the object is opaque; the receivedlight intensity will be very low, or almost zero (perhaps out of rangeof the sensing circuitry). If the object is translucent, however, thelight intensity will be quite high, but in general should be less thanthe peak value. In region 4, the probe is lifted and the light intensityrises sharply to a maximum value. In region 5, the probe is liftedfurther away from the object, and the light intensity decreases again.

As illustrated, two peak intensity values (discussed as P1 and P2 below)should be detected as the fiber optic pair moves to and from the objectat the critical height h_(c). If peaks P1 and P2 produced by a receivefiber optic are the same value, this generally is an indication that theprobe has been moved to and from the surface of the object to bemeasured in a consistent manner. If peaks P1 and P2 are of differentvalues, then these may be an indication that the probe was not moved toand from the surface of the object in a desired manner, or that thesurface is curved or textured, as described more fully herein. In such acase, the data may be considered suspect and rejected. In addition,peaks P1 and P2 for each of the perimeter fiber optics (see, e.g., FIG.2) should occur at the same critical height (assuming the geometricattributes of the perimeter fiber optics, such as aperture, diameter andspacing from the source fiber optic, etc). Thus, the perimeter fiberoptics of a probe moved in a consistent, perpendicular manner to andfrom the surface of the object being measured should have peaks P1 andP2 that occur at the same critical height. Monitoring receiver fibersfrom the perimeter receiver fiber optics and looking for simultaneous(or near simultaneous, e.g., within a predetermined range) peaks P1 andP2 provides a mechanism for determining if the probe is held at adesired perpendicular angle with respect to the object being measured.

In addition, the relative intensity level in region 3 serves as anindication of the level of translucency of the object being measured.Again, such principles generally are applicable to the totality ofreceiver fiber optics in the probe (see, e.g., fibers 7 of FIGS. 1 and3). Based on such principles, measurement techniques in accordance withthe present invention will now be described.

FIG. 6 is a flow chart illustrating a measuring technique in accordancewith the present invention. Step 49 indicates the start or beginning ofa color measurement. During step 49, any equipment initialization,diagnostic or setup procedures may be performed. Audio or visualinformation or other indicia may be given to the operator to inform theoperator that the system is available and ready to take a measurement.Initiation of the color measurement commences by the operator moving theprobe towards the object to be measured, and may be accompanied by, forexample, activation of switch 17 (see FIG. 1).

In step 50, the system on a continuing basis monitors the intensitylevels for the receiver fiber optics (see, e.g., fibers 7 of FIG. 1). Ifthe intensity is rising, step 50 is repeated until a peak is detected.If a peak is detected, the process proceeds to step 52. In step 52,measured peak intensity P1, and the time at which such peak occurred,are stored in memory (such as in memory included as a part ofmicroprocessor 10), and the process proceeds to step 54. In step 54, thesystem continues to monitor the intensity levels of the receiver fiberoptics. If the intensity is falling, step 54 is repeated. If a “valley”or plateau is detected (i.e., the intensity is no longer falling, whichgenerally indicates contact or near contact with the object), then theprocess proceeds to step 56. In step 56, the measured surface intensity(IS) is stored in memory, and the process proceeds to step 58. In step58, the system continues to monitor the intensity levels of the receiverfibers. If the intensity is rising, step 58 is repeated until a peak isdetected. If a peak is detected, the process proceeds to step 60. Instep 60, measured peak intensity P2, and the time at which such peakoccurred, are stored in memory, and the process proceeds to step 62. Instep 62, the system continues to monitor the intensity levels of thereceiver fiber optics. Once the received intensity levels begin to fallfrom peak P2, the system perceives that region 5 has been entered (see,e.g., FIG. 5A), and the process proceeds to step 64.

In step 64, the system, under control of microprocessor 10, may analyzethe collected data taken by the sensing circuitry for the variousreceiver fiber optics. In step 64, peaks P1 and P2 of one or more of thevarious fiber optics may be compared. If any of peaks P1 and P2 for anyof the various receiver fiber optics have unequal peak values, then thecolor data may be rejected, and the entire color measuring processrepeated. Again, unequal values of peaks P1 and P2 may be indicative,for example, that the probe was moved in a non-perpendicular orotherwise unstable manner (i.e., angular or lateral movement), and, forexample, peak P1 may be representative of a first point on the object,while peak P2 may be representative of a second point on the object. Asthe data is suspect, in a preferred embodiment of the present invention,color data taken in such circumstances are rejected in step 64.

If the data are not rejected in step 64, the process proceeds to step66. In step 66, the system analyzes the data taken from theneutral-density-filtered receivers from each of the perimeter fiberoptics (e.g., R1 to R3 of FIG. 2). If the peaks of the perimeter fiberoptics did not occur at or about the same point in time, this may beindicative, for example, that the probe was not held perpendicular tothe surface of the object being measured. As non-perpendicular alignmentof the probe with the surface of the object being measured may causesuspect results, in a preferred embodiment of the present invention,color data taken in such circumstances are rejected in step 66. In onepreferred embodiment, detection of simultaneous or near simultaneouspeaking (peaking within a predetermined range of time) serves as anacceptance criterion for the data, as perpendicular alignment generallyis indicated by simultaneous or near simultaneous peaking of theperimeter fiber optics. In other embodiments, step 66 includes ananalysis of peak values P1 and P2 of the perimeter fiber optics. In suchembodiments, the system seeks to determine if the peak values of theperimeter fiber optics (perhaps normalized with any initial calibrationdata) arc equal within a defined range. If the peak values of theperimeter fiber optics are within the defined range, the data may beaccepted, and if not, the data may be rejected In still otherembodiments, a combination of simultaneous peaking and equal valuedetection are used as acceptance/rejection criteria for the color data,and/or the operator may have the ability (such as through key padswitches 12) to control one or more of the acceptance criteria ranges.With such capability, the sensitivity of the system may be controllablyaltered by the operator depending upon the particular application andoperative environment, etc.

If the data are not rejected in step 66, the process proceeds to step68. In step 68, the color data may be processed in a desired manner toproduce output color measurement data. For example, such data may benormalized in some manner, or adjusted based on temperature ancompensation or other data detected by the system. The data also may beconverted to different display or other formats, depending on theintended use of the color data. In addition, the data indicative of thetranslucence of the object also may be quantified and/or displayed instep 68. After step 68, the process may proceed to starting step 49, orthe process may be terminated, etc.

In accordance with the process illustrated in FIG. 6, three lightintensity values (P1, P2 and IS) are stored per receiver fiber optic tomake color and translucency measurements. If stored peak values P1 andP2 are not equal (for some or all of the receivers), this is anindication that the probe was not held steady over one area, and thedata may be rejected (in other embodiments, the data may not berejected, although the resulting data may be used to produce an averageof the measured color data). In addition, peak values P1 and P2 for thethree neutral density perimeter fiber optics should be equal orapproximately equal; if this is not the case, then this is an indicationthat the probe was not held perpendicular or a curved surface is beingmeasured. In other embodiments, the system attempts to compensate forcurved surfaces and/or non-perpendicular angles. In any event, if thesystem cannot make a color measurement, or if the data is rejectedbecause peak values P1 and P2 are unequal to an unacceptable degree,then the operator is notified so that another measurement or otheraction may be taken (such as adjust the sensitivity).

With a system constructed and operating as described above, colormeasurements may be taken of an object, with accepted color data havingheight and angular dependencies removed. Data not taken at the criticalheight, or data not taken with the probe perpendicular to the surface ofthe object being measured, etc., are rejected in a preferred embodimentof the present invention. In other embodiments, data received from theperimeter fiber optics may be used to calculate the angle of the probewith respect to the surface of the object being measured, and in suchembodiments non-perpendicular or curved surface color data may becompensated instead of rejected. It also should be noted that peakvalues P1 and P2 for the neutral density perimeter fiber optics providea measure of the luminance (gray value) of the surface of the objectbeing measured, and also may serve to quantify the color value.

The translucency of the object being measured may be quantified as aratio or percentage, such as, for example, (IS/P1)×100%. In otherembodiments, other methods of quantifying translucency data provided inaccordance with the present invention are utilized.

In another particular aspect of the present invention, data generated inaccordance with the present invention may be used to implement anautomated material mixing/generation machine. Certain objects/materials,such as dental prostheses, are made from porcelain or otherpowders/materials that may be combined in the correct ratios to form thedesired color of the object/prosthesis. Certain powders often containpigments that generally obey Beer's law and/or act in accordance withKubelka-Munk equations when mixed in a recipe. Color and other datataken from a measurement in accordance with the present invention may beused to determine or predict desired quantities of pigment or othermaterials for the recipe. Porcelain powders and other materials areavailable in different colors, opacities, etc. Certain objects, such asdental prostheses, may be layered to simulate the degree of translucencyof the desired object (such as to simulate a human tooth). Datagenerated in accordance with the present invention also may be used todetermine the thickness and position of the porcelain or other materiallayers to more closely produce the desired color, translucency, surfacecharacteristics, etc. In addition, based on fluorescence data for thedesired object, the material recipe may be adjusted to include a desiredquantity of fluorescing-type material. In yet other embodiments, surfacecharacteristics (such as texture) information (as more fully describedherein) may be used to add a texturing material to the recipe, all ofwhich may be carried out in accordance with the present invention.

For more information regarding such pigment-material recipe typetechnology, reference may be made to: “The Measurement of Appearance,”Second Edition, edited by Hunter and Harold, copyright 1987; “Principlesof Color Technology,” by Billmeyer and Saltzman, copyright 1981; and“Pigment Handbook,” edited by Lewis, copyright 1988. All of theforegoing are believed to have been published by John Wiley & Sons,Inc., New York, N.Y., and all of which are hereby incorporated byreference.

In certain operative environments, such as dental applications,contamination of the probe is of concern. In certain embodiments of thepresent invention, implements to reduce such contamination are provided.

FIGS. 7A and 7B illustrate a protective cap that may be used to fit overthe end of probe tip 1. Such a protective cap consists of body 80, theend of which is covered by optical window 82, which in a preferredembodiment consists of a structure having a thin sapphire window. In apreferred embodiment, body 80 consists of stainless steel. Body 80 fitsover the end of probe tip 1 and may be held into place by, for example,indentations formed in body 80, which fit with ribs 84 (which may be aspring clip or other retainer) formed on probe tip 1. In otherembodiments, other methods of affixing such a protective cap to probetip 1 are utilized. The protective cap may be removed from probe tip 1and sterilized in a typical autoclave, hot steam or other sterilizingsystem.

The thickness of the sapphire window should be less than the criticalheight of the probe in order to preserve the ability to detect peakingin accordance with the present invention. It also is believed thatsapphire windows may be manufactured in a reproducible manner, and thusany light attenuation from one cap to another may be reproducible. Inaddition, any distortion of the color measurements produced by thesapphire window may be calibrated out by microprocessor 10.

Similarly, in other embodiments body 80 has a cap with a hole in thecenter (as opposed to a sapphire window), with the hole positioned overthe fiber optic source/receivers. The cap with the hole serves toprevent the probe from coming into contact with the surface, therebyreducing the risk of contamination.

FIGS. 8A and 8B illustrate another embodiment of a removable probe tipthat may be used to reduce contamination in accordance with the presentinvention. As illustrated in FIG. 8A, probe tip 88 is removable, andincludes four (or a different number, depending upon the application)fiber optic connectors 90, which are positioned within optical guard 92coupled to connector 94. Optical guard 92 serves to prevent “cross talk”between adjacent fiber optics. As illustrated in FIG. 8B, in thisembodiment removable tip 88 is secured in probe tip housing 93 by way ofspring clip 96 (other removable retaining implements are utilized inother embodiments). Probe tip housing 93 may be secured to baseconnector 95 by a screw or other conventional fitting. It should benoted that, with this embodiment, different size tips may be providedfor different applications, and that an initial step of the process maybe to install the properly-sized (or fitted tip) for the particularapplication. Removable tip 88 also may be sterilized in a typicalautoclave, hot steam or other sterilizing system. In addition, theentire probe tip assembly is constructed so that it may be readilydisassembled for cleaning or repair.

With reference to FIG. 9, a tristimulus embodiment of the presentinvention will now be described. In general, the overall system depictedin FIG. 1 and discussed in detail elsewhere herein may be used with thisembodiment. FIG. 9 illustrates a cross section of the probe tip fiberoptics used in this embodiment

Probe tip 100 includes central source fiber optic 106, surrounded by(and spaced apart from) three perimeter receiver fiber optics 104 andthree color receiver fiber optics 102. Three perimeter receiver fiberoptics 104 are optically coupled to neutral density filters and serve asheight/angle sensors in a manner analogous to the embodiment describeabove. Three color receiver fiber optics are optically coupled tosuitable tristimulus filters, such as red, green and blue filters. Withthis embodiment, a measurement may be made of tristimulus color valuesof the object, and the process described with reference to FIG. 6generally is applicable to this embodiment. In particular, perimeterfiber optics 104 may be used to detect simultaneous peaking or otherwisewhether the probe is perpendicular to the object being measured. Inaddition, taking color measurement data at the critical height also maybe used with this embodiment.

FIG. 10A illustrates an embodiment of the present invention, similar tothe embodiment discussed with reference to FIG. 9. Probe tip 100includes central source fiber optic 106, surrounded by (and spaced apartfrom) three perimeter receiver fiber optics 104 and a plurality of colorreceiver fiber optics 102. The number of color receiver fiber optics102, and the filters associated with such receiver fiber optics 102, maybe chosen based upon the particular application. As with the embodimentof FIG. 9, the process described with reference to FIG. 6 generally isapplicable to this embodiment.

FIG. 10B illustrates an embodiment of the present invention in whichthere are a plurality of receiver fiber optics that surround centralsource fiber optic 240. The receiver fiber optics are arranged in ringssurrounding the central source fiber optic. FIG. 10B illustrates threerings of receiver fiber optics (consisting of fiber optics 242, 244 and246, respectively), in which there are six receiver fiber optics perring. The rings may be arranged in successive larger circles asillustrated to cover the entire area of the end of the probe, with thedistance from each receiver fiber optic within a given ring to thecentral fiber optic being equal (or approximately so). Central fiberoptic 240 is utilized as the light source fiber optic and is connectedto the light source in a manner similar to light source fiber optic 5illustrated in FIG. 1.

The plurality of receiver fiber optics are each coupled to two or morefiber optics in a manner similar to the arrangement illustrated in FIG.1 for splicing connector 4. One fiber optic from such a splicingconnector for each receiver fiber optic passes through a neutral densityfilter and then to light sensor circuitry similar to the light sensorcircuitry illustrated in FIG. 3. A second fiber optic from the splicingconnector per receiver fiber optic passes through a Sharp CuttingWrattan Gelatin Filter and then to light sensor circuitry as discussedelsewhere herein. Thus, each of the receiver fiber optics in the probetip includes both color measuring elements and neutral light measuringor “perimeter” elements.

FIG. 10D illustrates the geometry of probe 260 (such as described above)illuminating an area on flat diffuse surface 272. Probe 260 createslight pattern 262 that is reflected diffusely from surface 272 inuniform hemispherical pattern 270. With such a reflection pattern, thereflected light that is incident upon the receiving elements in theprobe will be equal (or nearly equal) for all elements if the probe isperpendicular to the surface as described above herein.

FIG. 10C illustrates a probe illuminating rough surface 268 or a surfacethat reflects light spectrally. Spectral reflected light will exhibithot spots or regions 266 where the reflected light intensity isconsiderably greater than it is on other areas 264. The reflected lightpattern will be uneven when compared to a smooth surface as illustratein FIG. 10D.

Since a probe as illustrated in FIG. 10B has a plurality of receiverfiber optics arranged over a large surface area, the probe may beutilized to determine the surface texture of the surface as well asbeing able to measure the color and translucency of the surface asdescribed earlier herein. If the light intensity received by thereceiver fiber optics is equal for all fiber optics within a given ringof receiver fiber optics, then generally the surface is diffuse andsmooth. If, however, the light intensity of receiver fibers in a ringvaries with respect to each other, then generally the surface rough orspectral. By comparing the light intensities measured within receiverfiber optics in a given ring and from ring to ring, the texture andother characteristics of the surface may be quantified.

FIG. 11 illustrates an embodiment of the present invention in whichlinear optical sensors and a color gradient filter are utilized insteadof light sensors 8 (and filters 22, etc.). Receiver fiber optics 7,which may be optically coupled to probe tip 1 as with the embodiment ofFIG. 1, are optically coupled to linear optical sensor 112 through colorgradient filter 110. In this embodiment, color gradient filter 110 mayconsist of series of narrow strips of cut-off type filters on atransparent or open substrate, which are constructed so as topositionally correspond to the sensor areas of linear optical sensor112. An example of a commercially available linear optical sensor 112 isTexas Instruments part number TSL213, which has 61 photo diodes in alinear array. Light receiver fiber optics 7 are arranged correspondinglyin a line over linear optical sensor 112. The number of receiver fiberoptics may be chosen for the particular application, so long as enoughare included to more or less evenly cover the full length of colorgradient filter 110. With this embodiment, the light is received andoutput from receiver fiber optics 7, and the light received by linearoptical sensor 112.is integrated for a short period of time (determinedby the light intensity, filter characteristics and desired accuracy).The output of linear array sensor 112 is digitized by ADC 114 and outputto microprocessor 116 (which may the same processor as microprocessor 10or another processor).

In general, with the embodiment of FIG. 11, perimeter receiver fiberoptics may be used as with the embodiment of FIG. 1, and in general theprocess described with reference to FIG. 6 is applicable to thisembodiment.

FIG. 12 illustrates an embodiment of the present invention in which amatrix optical sensor and a color filter grid are utilized instead oflight sensors 8 (and filters 22, etc.). Receiver fiber optics 7, whichmay be optically coupled to probe tip 1 as with the embodiment of FIG.1, are optically coupled to matrix optical sensor 122 through filtergrid 120. Filter grid 120 is a filter array consisting of a number ofsmall colored spot filters that pass narrow bands of visible light.Light from receiver fiber optics 7 pass through corresponding filterspots to corresponding points on matrix optical sensor 122. In thisembodiment, matrix optical sensor 122 may be a monochrome optical sensorarray, such as CCD-type or other type of light sensor element such asmay be used in a video camera The output of matrix optical sensor 122 isdigitized by ADC 124 and output to microprocessor 126 (which may thesame processor as microprocessor 10 or another processor). Under controlof microprocessor 126, matrix optical sensor 126 collects color datafrom receiver fiber optics 7 through color filter grid 120.

In general, with the embodiment of FIG. 12, perimeter receiver fiberoptics may be used as with the embodiment of FIG. 1, and in general theprocess described with reference to FIG. 6 also is applicable to thisembodiment.

As will be clear from the foregoing description, with the presentinvention a variety of types of spectral color photometers (ortristimulus-type calorimeters) may be constructed, with perimeterreceiver fiber optics used to collect color data essentially free fromheight and angular deviations. In addition, in certain embodiments, thepresent invention enables color measurements to be taken at a criticalheight from the surface of the object being measured, and thus colordata may be taken without physical contact with the object beingmeasured (in such embodiments, the color data is taken only by passingthe probe through region I and into region 2, but without necessarilygoing into region 3 of FIGS. 5A and 5B). Such embodiments may beutilized if contact with the surface is undesirable in a particularapplication. In the embodiments described earlier, however, physicalcontact (or near physical contact) of the probe with the object mayallow all five regions of FIGS. 5A and 5B to be utilized, therebyenabling color measurements to be taken such that translucencyinformation also may be obtained. Both types of embodiments generallyare within the scope of the invention described herein.

Additional description will now be provided with respect to cut-offfilters of de type described in connection with the preferredembodiment(s) of FIGS. 1 and 3 (such as filters 22 of FIG. 3). FIG. 13Aillustrates the properties of a single Kodak Sharp Cutting WrattenGelatin Filter discussed in connection with FIG. 3. Such a cut-offfilter passes light below a cut-off frequency (i.e., above a cut-offwavelength). Such filters may be manufactured to have a wide range ofcut-off frequencies/wavelengths. FIG. 13B illustrates a number of suchfilters, twelve in a preferred embodiment, with cut-offfrequencies/wavelengths chosen so that essentially the entire visibleband is covered by the collection of cut-off filters.

FIGS. 14A and 14B illustrate exemplary intensity measurements using acut-off filter arrangement such as illustrated in FIG. 13B, first in thecase of a white surface being measured (FIG. 14A), and also in the caseof a blue surface being measured (FIG. 14B). As illustrated in FIG. 14A,in the case of a white surface, the neutrally filtered perimeter fiberoptics, which are used to detect height and angle, etc., generally willproduce the highest intensity (although this depends at least in partupon the characteristics of the neutral density filters). As a result ofthe stepped cut-off filtering provided by filters having thecharacteristics illustrated in FIG. 13B, the remaining intensities willgradually decrease in value as illustrated in FIG. 14A. In the case of ablue surface, the intensities will decrease in value generally asillustrated in FIG. 14B. Regardless of the surface, however, theintensities out of the filters will always decrease in value asillustrated, with the greatest intensity value being the output of thefilter having the lowest wavelength cut-off value (i.e., passes allvisible light up to blue), and the lowest intensity value being theoutput of the filter having the highest wavelength cutoff (i.e., passesonly red visible light). As will be understood from the foregoingdescription, any color data detected that does not fit the decreasingintensity profiles of FIGS. 14A and 14B may be detected as anabnormality, and in certain embodiments detection of such a conditionresults in data rejection, generation of an error message or initiationof a diagnostic routine, etc.

Reference should be made to the FIGS. 1 and 3 and the relateddescription for a detailed discussion of how such a cut-off filterarrangement may be utilized in accordance with the present invention.

FIG. 15 is a flow chart illustrating audio tones that may be used incertain preferred embodiments of the present invention. It has beendiscovered that audio tones (such as tones, beeps, voice or the likesuch as will be described) present a particularly useful and instructivemeans to guide an operator in the proper use of a color measuring systemof the type described herein.

The operator may initiate a color measurement by activation of a switch(such as switch 17 of FIG. 1) at step 150. Thereafter, if the system isready (set-up, initialized, calibrated, etc.), a lower-the-probe tone isemitted (such as through speaker 16 of FIG. 1) at step 152. The systemattempts to detect peak intensity P1 at step 154. If a peak is detected,at step 156 a determination is made whether the measured peak P1 meetsthe applicable criteria (such as discussed above in connection withFIGS. 5A, SB and 6). If the measured peak P1 is accepted, a first peakacceptance tone is generated at step 160. If the measured peak P1 is notaccepted, an unsuccessful tone is generated at step 158, and the systemmay await the operator to initiate a further color measurement. Assumingthat the first peak was accepted, the system attempts to detect peakintensity P2 at step 362. If a second peak is detected, at step 164 adetermination is so made whether the measured peak P2 meets theapplicable criteria If the measured peak P2 is accepted the processproceeds to color calculation step 166 (in other embodiments, a secondpeak acceptance tone also is generated at step 166). If the measuredpeak P2 is not accepted, an unsuccessful tone is generated at step 158,and the system may await the operator to initiate a further colormeasurement. Assuming that the second peak was accepted, a colorcalculation is made at step 166 (such as, for example, microprocessor 10of FIG. 1 processing the data output from light sensors 8, etc.). Atstep 168, a determination is made whether the color calculation meetsthe applicable criteria. If the color calculation is accepted, asuccessful tone is generated at step 170. If the color calculation isnot accepted, an unsuccessful tone is generated at step 158, and thesystem may await the operator to initiate a further color measurement.

With unique audio tones presented to an operator in accordance with theparticular operating state of the system, the operator's use of thesystem may be greatly facilitated. Such audio information also tends toincrease operator satisfaction and skill level, as, for example,acceptance tones provide positive and encouraging feedback when thesystem is operated in a desired manner.

As will be apparent to those skilled in the art, certain refinements maybe made in accordance with the present invention. For example, a centrallight source fiber optic is utilized in certain preferred embodiments,but other light source arrangements (such as a plurality of light sourcefibers, etc.). In addition, lookup tables are utilized for variousaspects of the present invention, but polynomial type calculations couldsimilarly be employed. Thus, although various preferred embodiments ofthe present invention have been disclosed for illustrative purposes,those skilled in the art will appreciate that various modifications,additions and/or substitutions are possible without departing from thescope and spirit of the present invention as disclosed in the claims.

Reference is also made to copending application Ser. No. 08/582,054,filed Jan. 2, 1996, for “Apparatus and Method for Measuring the Color ofTeeth,” by the inventors hereof, which is hereby incorporated byreference.

What is claimed is:
 1. A method of determining a characteristic of anobject or material comprising the steps of: receiving light from theobject or material; coupling received light to one or more sensors;generating at least one signal having a frequency proportional to thelight intensity received by the one or more sensors; and determining thecharacteristic based on the at least one signal; wherein the lightpasses through a filter prior to being coupled to one or more of thesensors.
 2. The method of claim 1, wherein the at least one signalcomprises a digital signal.
 3. The method of claim 2, wherein thedigital signal comprises a TTL or CMOS digital signal.
 4. The method ofclaim 1, wherein the signal comprises an asynchronous signal of afrequency dependent upon the intensity of the received light.
 5. Themethod of claim 1, wherein the one or more sensors comprise a pluralityof light to frequency converter sensing elements.
 6. The method of claim1, wherein the characteristic comprises a spectral analysis based onlight received from the object or material.
 7. The method of claim 1,wherein the step of generating at least one signal having a frequencyproportional to the light intensity received by the one or more sensorscomprises integrating light coupled to the one or more sensors with anintegrator.
 8. The method of claim 1, wherein the sensors comprise aphoto detector.
 9. The method of claim 8, wherein the photo detectorcomprises a photo diode.
 10. The method of claim 8, wherein the photodetector comprises a photo diode array.
 11. A method of determining acharacteristic of an object or material comprising the steps of:receiving light from the object or material; coupling received light toa plurality of sensors; generating a plurality of signals having afrequency proportional to the light intensity received by the sensors;and determining the characteristic based on the signals; wherein thelight passes through a filter prior to being coupled to the sensors,wherein spectral characteristics are determined based on measuring aperiod of a plurality of the signals.
 12. The method of claim 11,wherein the signals comprise TTL or CMOS digital signals.
 13. The methodof claim 11, wherein the signals comprise asynchronous signals of afrequency dependent upon the intensity of the received light.
 14. Themethod of claim 11, wherein the plurality of sensors comprise aplurality of light to frequency converter sensing elements.
 15. Themethod of claim 11, wherein the filter comprises a plurality of filterportions having a wavelength dependent optical transmission property.16. The method of claim 11, wherein the characteristic comprises aspectral analysis based on light received from the object or material.17. The method of claim 11, wherein the filter comprises a plurality ofcut-off filter elements.
 18. The method of claim 11, wherein the filtercomprises a color gradient filter.
 19. The method of claim 11, whereinthe filter comprises a filter grid.
 20. The method of claim 11, whereinthe received light is spectrally analyzed without using a diffractiongrating.
 21. The method of claim 11, wherein the light is received by aprobe, wherein a plurality of measurements are taken at a plurality ofdistances of the probe with respect to the object or material.
 22. Themethod of claim 11, wherein a probe having one or more light sourcesprovides light to the object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material.
 23. The method of claim 22, wherein one or moresensors determine a distance of the probe with respect to the object ormaterial.
 24. The method of claim 22, wherein one or more sensorsdetermine an angle of the probe with respect to the object or material.25. The method of claim 22, wherein one or more sensors determine adistance and an angle of the probe with respect to the object ormaterial.
 26. The method of claim 11, wherein the step of generating atleast one signal having a frequency proportional to the light intensityreceived by the one or more sensors comprises integrating light coupledto the one or more sensors with an integrator.
 27. The method of claim11, wherein the sensors comprise a photo detector.
 28. The method ofclaim 27, wherein the photo detector comprises a photo diode.
 29. Themethod of claim 27, wherein the photo detector comprises a photo diodearray.
 30. A method of determining a characteristic of an object ormaterial comprising the steps of: receiving light from the object ormaterial; coupling received light to one or more sensors; generating atleast one signal having a frequency proportional to the light intensityreceived by the one or more sensors; and determining the characteristicbased on the at least one signal; wherein the light passes through afilter prior to being coupled to one or more of the sensors, wherein thefilter comprises a plurality of filter portions having a wavelengthdependent optical transmission property.
 31. A method of determining acharacteristic of an object or material comprising the steps of:receiving light from the object or material; coupling received light toone or more sensors; generating at least one signal having a frequencyproportional to the light intensity received by the one or more sensors;and determining the characteristic based on the at least one signal;wherein the light passes through a filter prior to being coupled to oneor more of the sensors, wherein the filter comprises a plurality ofcut-off filter elements.
 32. A method of determining a characteristic ofan object or material comprising the steps of: receiving light from theobject or material; coupling received light to one or more sensors;generating at least one signal having a frequency proportional to thelight intensity received by the one or more sensors; and determining thecharacteristic based on the at least one signal; wherein the lightpasses through a filter prior to being coupled to one or more of thesensors, wherein the filter comprises a color gradient filter.
 33. Amethod of determining a characteristic of an object or materialcomprising the steps of: receiving light from the object or material;coupling received light to one or more sensors; generating at least onesignal having a frequency proportional to the light intensity receivedby the one or more sensors; and determining the characteristic based onthe at least one signal; wherein the light passes through a filter priorto being coupled to one or more of the sensors, wherein the filtercomprises a filter grid.
 34. A method of determining a characteristic ofan object or material comprising the steps of: receiving light from theobject or material; coupling received light to one or more sensors;generating at least one signal having a frequency proportional to thelight intensity received by the one or more sensors; and determining thecharacteristic based on the at least one signal; wherein the lightpasses through a filter prior to being coupled to one or more of thesensors, wherein the received light is spectrally analyzed without usinga diffraction grating.
 35. A method of determining a characteristic ofan object or material comprising the steps of: receiving light from theobject or material; coupling received light to one or more sensors;generating at least one signal having a frequency proportional to thelight intensity received by the one or more sensors; and determining thecharacteristic based on the at least one signal; wherein the light isreceived by a probe, wherein a plurality of measurements are taken at aplurality of distances of the probe with respect to the object ormaterial.
 36. A method of determining a characteristic of an object ormaterial comprising the steps of: receiving light from the object ormaterial; coupling received light to one or more sensors; generating atleast one signal having a frequency proportional to the light intensityreceived by the one or more sensors; and determining the characteristicbased on the at least one signal; wherein a probe having one or morelight sources provides light to the object or material, wherein lightfrom the one or more light sources is received by the one or more lightreceivers from the object or material.
 37. The method of claim 36,wherein one or more sensors determine a distance of the probe withrespect to the object or material.
 38. The method of claim 36, whereinone or more sensors determine an angle of the probe with respect to theobject or material.
 39. The method of claim 36, wherein one or moresensors determine a distance and an angle of the probe with respect tothe object or material.
 40. A method comprising the steps of: producingrelative movement between a probe and an object or material, wherein theprobe provides light provided by one or more light sources to the objector material and receives light from the object or material by one ormore light receivers; coupling light received be the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter; and determining the optical characteristics including at leastspectral characteristics of the object or material; wherein theplurality of optical sensors comprise a plurality of light to frequencyconverter sensing elements.
 41. A method comprising the steps of:producing relative movement between a probe and an object or material,wherein the probe provides light provided by one or more light sourcesto the object or material and receives light from the object or materialby one or more light receivers; coupling light received by the one ormore light receivers to a plurality of optical sensors through a colorgradient filter; and determining the optical characteristics includingat least spectral characteristics of the object or material; wherein thedetermining step comprises generating at least one signal having afrequency proportional to the light intensity received by the opticalsensors; and determining the optical characteristics based on the atleast one signal.
 42. The method of claim 41, wherein the at least onesignal comprises a digital signal.
 43. The method of claim 42, whereinthe digital signal comprises a TTL or CMOS digital signal.
 44. Themethod of claim 41, wherein spectral characteristics are determinedbased on measuring a period of a plurality of digital signals producedby a plurality of optical sensors.
 45. The method of claim 41, whereinthe signal comprises an asynchronous signal of a frequency dependentupon the intensity of the received light.
 46. The method of claim 41,wherein the color gradient filter comprises a plurality of filterportions having a wavelength dependent optical transmission property.47. The method of claim 41, wherein the optical characteristics comprisea spectral analysis based on light received from the object or material.48. The method of claim 41, wherein the color gradient filter comprisesa plurality of cut-off filter elements.
 49. The method of claim 41,wherein the received light is spectrally analyzed without using adiffraction grating.
 50. A method comprising the steps of: producingrelative movement between a probe and an object or material, wherein theprobe provides light provided by one or more light sources to the objector material and receives light from the object or material by one ormore light receivers; coupling light received by the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter; and determining the optical characteristics including at leastspectral characteristics of the object or material; wherein theplurality of optical sensors comprise a matrix of sensors.
 51. A methodcomprising the steps of: producing relative movement between a probe andan object or material, wherein the probe provides light provided by oneor more light sources to the object or material and receives light fromthe object or material by one or more light receivers; coupling lightreceived by the one or more light receivers to a plurality of opticalsensors through a color gradient filter; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein a plurality of measurements are taken at aplurality of distances of the probe with respect to the object ormaterial.
 52. The method of claim 51, wherein the plurality of opticalsensors comprise a linear array of optical sensors.
 53. The method ofclaim 51, wherein the plurality of optical sensors comprise CCD sensingelements.
 54. A method comprising the steps of: producing relativemovement between a probe and an object or material, wherein the probeprovides light provided by one or more light sources to the object ormaterial and receives light from the object or material by one or morelight receivers; coupling light received by the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter; and determining the optical characteristics including at leastspectral characteristics of the object or material; wherein one or moreoptical sensors determine a distance of the probe with respect to theobject or material.
 55. The method of claim 54, wherein the plurality ofoptical sensors comprise an array of sensors.
 56. A method comprisingthe steps of: producing relative movement between a probe and an objector material, wherein the probe provides light provided by one or morelight sources to the object or material and receives light from theobject or material by one or more light receivers; coupling lightreceived by the one or more light receivers to a plurality of opticalsensors through a color gradient filter; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein one or more optical sensors determine anangle of the probe with respect to the object or material.
 57. A methodcomprising the steps of: producing relative movement between a probe andan object or material, wherein the probe provides light provided by oneor more light sources to the object or material and receives light fromthe object or material by one or more light receivers; coupling lightreceived by the one or more light receivers to a plurality of opticalsensors through a color gradient filter; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein one or more optical sensors determine adistance and an angle of the probe with respect to the object ormaterial.
 58. A method comprising the steps of: receiving light from anobject or material with one or more light receivers, the one or morelight receivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received be theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein the plurality of optical sensors comprise aplurality of light to frequency converter sensing elements.
 59. A methodcomprising the steps of: receiving light from an object or material withone or more light receivers, the one or more light receivers providinglight at a plurality of spaced apart receiver outputs; coupling thelight received by the one or more light receivers to a plurality ofoptical sensors through a color gradient filter, wherein the pluralityof optical sensors receive light received by the one or more lightreceivers from the plurality of spaced apart receiver outputs throughthe color gradient filter, wherein the plurality of spaced apartreceiver outputs, a plurality of portions of the color gradient filterand the plurality of optical sensors are positionally arranged in acorresponding manner; and determining the optical characteristicsincluding at least spectral characteristics of the object or material;wherein the determining step comprises generating at least one signalhaving a frequency proportional to the light intensity received by theone or more optical sensors; and determining the optical characteristicsbased on the at least one signal.
 60. The method of claim 59, whereinthe at least one signal comprises a digital signal.
 61. The method ofclaim 60, wherein the digital signal comprises a TTL or CMOS digitalsignal.
 62. The method of claim 59, wherein spectral characteristics aredetermined based on measuring a period of a plurality of digital signalsproduced by a plurality of optical sensors.
 63. The method of claim 59,wherein the signal comprises an asynchronous signal of a frequencydependent upon the intensity of the received light.
 64. The method ofclaim 59, wherein the plurality of optical sensors comprise a lineararray of optical sensors.
 65. The method of claim 59, wherein theplurality of optical sensors comprise an array of sensors.
 66. Themethod of claim 59, wherein the color gradient filter comprises aplurality of filter portions having a wavelength dependent opticaltransmission property.
 67. The method of claim 59, wherein the opticalcharacteristics comprise a spectral analysis based on light receivedfrom the object or material.
 68. The method of claim 59, wherein thecolor gradient filter comprises a plurality of cut-off filter elements.69. The method of claim 59, wherein the received light is spectrallyanalyzed without using a diffraction grating.
 70. The method of claim59, wherein a probe having one or more light sources provides light tothe object or material, wherein light from the one or more light sourcesis received by the one or more light receivers from the object ormaterial.
 71. A method comprising the steps of: receiving light from anobject or material with one or more light receivers, the one or morelight receivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein the plurality of optical sensors comprise amatrix of sensors.
 72. A method comprising the steps of: receiving lightfrom an object or material with one or more light receivers, the one ormore light receivers providing light at a plurality of spaced apartreceiver outputs; coupling the light received by the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter, wherein the plurality of optical sensors receive light receivedby the one or more light receivers from the plurality of spaced apartreceiver outputs through the color gradient filter, wherein theplurality of spaced apart receiver outputs, a plurality of portions ofthe color gradient filter and the plurality of optical sensors arepositionally arranged in a corresponding manner; and determining theoptical characteristics including at least spectral characteristics ofthe object or material; wherein the light is received by a probe,wherein a plurality of measurements are taken at a plurality ofdistances of the probe with respect to the object or material.
 73. Themethod of claim 72, wherein the plurality of optical sensors compriseCCD sensing elements.
 74. A method comprising the steps of: receivinglight from an object or material with one or more light receivers, theone or more light receivers providing light at a plurality of spacedapart receiver outputs; coupling the light received by the one or morelight receivers to a plurality of optical sensors through a colorgradient filter, wherein the plurality of optical sensors receive lightreceived by the one or more light receivers from the plurality of spacedapart receiver outputs through the color gradient filter, wherein theplurality of spaced apart receiver outputs, a plurality of portions ofthe color gradient filter and the plurality of optical sensors arepositionally arranged in a corresponding manner; and determining theoptical characteristics including at least spectral characteristics ofthe object or material; wherein a probe having one or more light sourcesprovides light to the object or material; wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein a plurality of measurements are taken ata plurality of distances of the probe with respect to the object ormaterial.
 75. A method comprising the steps of: receiving light from anobject or material with one or more light receivers, the one or morelight receivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein a probe having one or more light sourcesprovides light to the object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein one or more optical sensors determine adistance of the probe with respect to the object or material.
 76. Amethod comprising the steps of: receiving light from an object ormaterial with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of theobject or material; wherein a probe having one or more light sourcesprovides light to the object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein one or more optical sensors determine anangle of the probe with respect to the object or material.
 77. A methodcomprising the steps of: receiving light from an object or material withone or more light receivers, the one or more light receivers providinglight at a plurality of spaced apart receiver outputs; coupling thelight received by the one or more light receivers to a plurality ofoptical sensors through a color gradient filter, wherein the pluralityof optical sensors receive light received by the one or more lightreceivers from the plurality of spaced apart receiver outputs throughthe color gradient filter, wherein the plurality of spaced apartreceiver outputs, a plurality of portions of the color gradient filterand the plurality of optical sensors are positionally arranged in acorresponding manner; and determining the optical characteristicsincluding at least spectral characteristics of the object or material;wherein a probe having one or more light sources provides light to theobject or material, wherein light from the one or more light sources isreceived by the one or more light receivers from the object or material;wherein one or more optical sensors determine a distance and an angle ofthe probe with respect to the object or material.
 78. A methodcomprising the steps of: receiving light that is to be spectrallyanalyzed with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of thereceived light; wherein the plurality of optical sensors comprise aplurality of light to frequency converter sensing elements.
 79. A methodcomprising the steps of: receiving light that is to be spectrallyanalyzed with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of thereceived light; wherein the determining step comprises generating atleast one signal having a frequency proportional to the light intensityreceived by the one or more optical sensors; and determining the opticalcharacteristics based on the at least one signal.
 80. The method ofclaim 79, wherein the at least one signal comprises a digital signal.81. The method of claim 79, wherein the digital signal comprises a TTLor CMOS digital signal.
 82. The method of claim 79, wherein spectralcharacteristics are determined based on measuring a period of aplurality of digital signals produced by a plurality of optical sensors.83. The method of claim 79, wherein the signal comprises an asynchronoussignal of a frequency dependent upon the intensity of the receivedlight.
 84. The method of claim 79, wherein the plurality of opticalsensors comprise a linear array of optical sensors.
 85. The method ofclaim 79, wherein the plurality of optical sensors comprise an array ofsensors.
 86. The method of claim 79, wherein the color gradient filtercomprises a plurality of filter portions having a wavelength dependentoptical transmission property.
 87. The method of claim 79, wherein theoptical characteristics comprise a spectral analysis based on thereceived light.
 88. The method of claim 79, wherein the color gradientfilter comprises a plurality of cut-off filter elements.
 89. The methodof claim 79, wherein the received light is spectrally analyzed withoutusing a diffraction grating.
 90. The method of claim 79, wherein a probehaving one or more light sources provides light to an object ormaterial, wherein light from the one or more light sources is receivedby the one or more light receivers from the object or material.
 91. Amethod comprising the steps of: receiving light that is to be spectrallyanalyzed with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of thereceived light; wherein the plurality of optical sensors comprise amatrix of sensors.
 92. A method comprising the steps of: receiving lightthat is to be spectrally analyzed with one or more light receivers, theone or more light receivers providing light at a plurality of spacedapart receiver outputs; coupling the light received by the one or morelight receivers to a plurality of optical sensors through a colorgradient filter, wherein the plurality of optical sensors receive lightreceived by the one or more light receivers from the plurality of spacedapart receiver outputs through the color gradient filter, wherein theplurality of spaced apart receiver outputs, a plurality of portions ofthe color gradient filter and the plurality of optical sensors arepositionally arranged in a corresponding manner; and determining theoptical characteristics including at least spectral characteristics ofthe received light; wherein the light is received by a probe, wherein aplurality of measurements are taken at a plurality of distances of theprobe with respect to the object or material.
 93. The method of claim92, wherein the plurality of optical sensors comprise CCD sensingelements.
 94. A method comprising the steps of: receiving light that isto be spectrally analyzed with one or more light receivers, the one ormore light receivers providing light at a plurality of spaced apartreceiver outputs; coupling the light received by the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter, wherein the plurality of optical sensors receive light receivedby the one or more light receivers from the plurality of spaced apartreceiver outputs through the color gradient filter, wherein theplurality of spaced apart receiver outputs, a plurality of portions ofthe color gradient filter and the plurality of optical sensors arepositionally arranged in a corresponding manner; and determining theoptical characteristics including at least spectral characteristics ofthe received light; wherein a probe having one or more light sourcesprovides light to an object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein a plurality of measurements are taken ata plurality of distances of the probe with respect to the object ormaterial.
 95. A method comprising the steps of: receiving light that isto be spectrally analyzed with one or more light receivers, the one ormore light receivers providing light at a plurality of spaced apartreceiver outputs; coupling the light received by the one or more lightreceivers to a plurality of optical sensors through a color gradientfilter, wherein the plurality of optical sensors receive list receivedby the one or more light receivers from the plurality of spaced apartreceiver outputs through the color gradient filter, wherein theplurality of spaced apart receiver outputs, a plurality of portions ofthe color gradient filter and the plurality of optical sensors arepositionally arranged in a corresponding manner; and determining theoptical characteristics including at least spectral characteristics ofthe received light; wherein a probe having one or more light sourcesprovides light to an object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein one or more optical sensors determine adistance of the probe with respect to the object or material.
 96. Amethod comprising the steps of: receiving light that is to be spectrallyanalyzed with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of thereceived light; wherein a probe having one or more light sourcesprovides light to an object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein one or more optical sensors determine anangle of the probe with respect to the object or material.
 97. A methodcomprising the steps of: receiving light that is to be spectrallyanalyzed with one or more light receivers, the one or more lightreceivers providing light at a plurality of spaced apart receiveroutputs; coupling the light received by the one or more light receiversto a plurality of optical sensors through a color gradient filter,wherein the plurality of optical sensors receive light received by theone or more light receivers from the plurality of spaced apart receiveroutputs through the color gradient filter, wherein the plurality ofspaced apart receiver outputs, a plurality of portions of the colorgradient filter and the plurality of optical sensors are positionallyarranged in a corresponding manner; and determining the opticalcharacteristics including at least spectral characteristics of thereceived light; wherein a probe having one or more light sourcesprovides light to an object or material, wherein light from the one ormore light sources is received by the one or more light receivers fromthe object or material; wherein one or more optical sensors determine adistance and an angle of the probe with respect to the object ormaterial.
 98. A method comprising the steps of: receiving light with oneor more light receivers wherein the one or more light receivers receivelight to be spectrally analyzed; and coupling light received by the oneor more light receivers to an optical sensor through a color filter,wherein the color filter has a plurality of portions, wherein each ofthe plurality of portions has a wavelength dependent light transmissionproperty covering a predetermined band or bands of wavelengths, whereinthe predetermined bands of the plurality of portions cover apredetermined band of wavelengths to be spectrally analyzed whereinlight from the one or more light receivers is coupled to the pluralityof portions of the color filter, wherein the optical sensor has aplurality of sensing elements, wherein light received by the one or morelight receivers is coupled to the sensing elements through the pluralityof portions of the color filter; wherein light received by the one ormore light receivers is spectrally analyzed without using a diffractiongrating; wherein the optical sensor comprises a plurality of light tofrequency converter sensing elements.
 99. The method of claim 98,wherein the color filter comprises a plurality of cut-off filterelements.
 100. The method of claim 98, wherein the light is coupled tothe color filter through one or more fiber optics.
 101. The method ofclaim 98, wherein the predetermined bands comprise narrow bands ofwavelengths.
 102. The method of claim 98, wherein the plurality ofportions each comprise a filter element that passes light of a narrowband of wavelengths.
 103. The method of claim 98, wherein the receivedlight comprises light directed from a probe to an object, whereincharacteristics of the object are determined based on the spectrallyanalyzed light.
 104. The method of claim 98, wherein the optical sensorcomprises a spectrometer.
 105. The method of claim 98, wherein theoptical sensor comprises a colorimeter.
 106. The method of claim 98,wherein the optical sensor includes at least three separate sensorelements and produces spectral data in the form of a tristimulus dataoutput.
 107. The method of claim 98, wherein a probe having one or morelight sources provides light to an object or material, wherein lightfrom the one or more light sources is received by the one or more lightreceivers from the object or material.
 108. The method of claim 98,wherein the predetermined band of wavelengths to be spectrally analyzedcomprises substantially the visible band.
 109. The method of claim 98,wherein the plurality of sensing elements comprise an array of sensingelements.
 110. A method comprising the steps of: receiving light withone or more light receivers, wherein the one or more light receiversreceive light to be spectrally analyzed; and coupling light received bythe one or more light receivers to an optical sensor through a colorfilter, wherein the color filter has a plurality of portions, whereineach of the plurality of portions has a wavelength dependent lighttransmission property covering a predetermined band or bands ofwavelengths, wherein the predetermined bands of the plurality ofportions cover a predetermined band of wavelengths to be spectrallyanalyzed, wherein light from the one or more light receivers is coupledto the plurality of portions of the color filter, wherein the opticalsensor has a plurality of sensing elements, wherein light received bythe one or more light receivers is coupled to the sensing elementsthrough the plurality of portions of the color filter; wherein lightreceived by the one or more light receivers is spectrally analyzedwithout using a diffraction grating; wherein the optical sensorintegrates the received light.
 111. A method comprising the steps of:receiving light with one or more light receivers, wherein the one ormore light receivers receive light to be spectrally analyzed; andcoupling light received by the one or more light receivers to an opticalsensor through a color filter, wherein the color filter has a pluralityof portions, wherein each of the plurality of portions has a wavelengthdependent light transmission property covering a predetermined band orbands of wavelengths, wherein the predetermined bands of the pluralityof portions cover a predetermined band of wavelengths to be spectrallyanalyzed, wherein light from the one or more light receivers is coupledto the plurality of portions of the color filter, wherein the opticalsensor has a plurality of sensing elements, wherein light received bythe one or more light receivers is coupled to the sensing elementsthrough the plurality of portions of the color filter; wherein lightreceived by the one or more light receivers is spectrally analyzedwithout using a diffraction grating; wherein a probe having one or morelight sources provides light to an object or material, wherein lightfrom the one or more light sources is received by the one or more lightreceivers from the object or material.
 112. The method of claim 111,wherein the optical sensor comprises a linear array of photo detectors.113. The method of claim 112, wherein the linear array of photodetectors provides an output to an analog-to-digital converter.
 114. Themethod of claim 113, wherein the analog-to-digital converter provides anoutput to a processor.
 115. The method of claim 114, wherein theprocessor outputs spectral analysis data.
 116. The method of claim 111,wherein the sensing elements comprise a photo detector.
 117. The methodof claim 116, wherein the photo detector comprises a photo diode. 118.The method of claim 116, wherein the photo detector comprises a photodiode array.
 119. The method of claim 111, wherein the plurality ofsensing elements comprise CCD sensing elements.
 120. A method comprisingthe steps of: receiving light with one or more light receivers, whereinthe one or more light receivers receive light to be spectrally analyzed;and coupling light received by the one or more light receivers to anoptical sensor through a color filter, wherein the color filter has aplurality of portions, wherein each of the plurality of portions has awavelength dependent light transmission property covering apredetermined band or bands of wavelengths, wherein the predeterminedbands of the plurality of portions cover a predetermined band ofwavelengths to be spectrally analyzed, wherein light from the one ormore light receivers is coupled to the plurality of portions of thecolor filter, wherein the optical sensor has a plurality of sensingelements, wherein light received by the one or more light receivers iscoupled to the sensing elements through the plurality of portions of thecolor filter; wherein light received by the one or more light receiversis spectrally analyzed without using a diffraction grating; wherein aprobe having one or more light sources provides light to an object ormaterial, wherein light from the one or more light sources is receivedby the one or more light receivers from the object or material; whereinone or more optical sensors determine an angle of the probe with respectto the object or material.
 121. A method comprising the steps of:receiving light with one or more light receivers, wherein the one ormore light receivers receive light to be spectrally analyzed; andcoupling light received by the one or more light receivers to an opticalsensor through a color filter, wherein the color filter has a pluralityof portions, wherein each of the plurality of portions has a wavelengthdependent light transmission property covering a predetermined band orbands of wavelengths, wherein the predetermined bands of the pluralityof portions cover a predetermined band of wavelengths to be spectrallyanalyzed, wherein light from the one or more light receivers is coupledto the plurality of portions of the color filter, wherein the opticalsensor has a plurality of sensing elements, wherein light received bythe one or more light receivers is coupled to the sensing elementsthrough the plurality of portions of the color filter; wherein lightreceived by the one or more light receivers is spectrally analyzedwithout using a diffraction grating; wherein a probe having one or morelight sources provides light to an object or material, wherein lightfrom the one or more light sources is received by the one or more lightreceivers from the object or material; wherein one or more opticalsensors determine a distance and an angle of the probe with respect tothe object or material.
 122. A method comprising the steps of: receivinglight with one or more light receivers, wherein the one or more lightreceivers receive light to be spectrally analyzed; and coupling lightreceived by the one or more light receivers to an optical sensor througha color filter, wherein the color filter has a plurality of portions,wherein each of the plurality of portions has a wavelength dependentlight transmission property covering a predetermined band or bands ofwavelengths, wherein the predetermined bands of the plurality ofportions cover a predetermined band of wavelengths to be spectrallyanalyzed, wherein light from the one or more light receivers is coupledto the plurality of portions of the color filter, wherein the opticalsensor has a plurality of sensing elements, wherein light received bythe one or more light receivers is coupled to the sensing elementsthrough the plurality of portions of the color filter; wherein lightreceived by the one or more light receivers is spectrally analyzedwithout using a diffraction grating; wherein the plurality of sensingelements comprise a matrix of sensing elements.